<?xml version="1.0" encoding="UTF-8"?>
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<dc:dc xmlns:dc="http://purl.org/dc/elements/1.1/" xmlns:invenio="http://invenio-software.org/elements/1.0" xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance" xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/ http://www.openarchives.org/OAI/2.0/oai_dc.xsd"><dc:identifier>doi:10.1021/acs.cgd.3c00160</dc:identifier><dc:language>eng</dc:language><dc:creator>Šterbinská, Slavomíra</dc:creator><dc:creator>Holub, Mariia</dc:creator><dc:creator>Cižmár, Erik</dc:creator><dc:creator>Cernák, Juraj</dc:creator><dc:creator>Falvello, Lawrence Rocco</dc:creator><dc:creator>Tomás, Milagros</dc:creator><dc:title>An Old Crystallization Technique as a Fast, Facile, and Adaptable Method for Obtaining Single Crystals of Unstable “Li2TCNQF4” and New Compounds of TCNQ or TCNQF4: Syntheses, Crystal Structures, and Magnetic Properties</dc:title><dc:identifier>ART-2023-135294</dc:identifier><dc:description>Detailed structural information is essential for understanding the properties of TCNQ and TCNQF4 compounds (TCNQ = 7,7,8,8-tetracyanoquinodimethane; TCNQF4 = 2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane). The ineludible requirement of obtaining crystals of a size and quality sufficient to yield a successful X-ray diffraction analysis has been challenging to satisfy because of the instability of many of these compounds in solution. Crystals of two new complexes of TCNQ, [trans-M(2ampy)2(TCNQ)2] [M = Ni (1), Zn (2); 2ampy = 2-aminomethylpyridine], as well as unstable [Li2(TCNQF4)(CH3CN)4]·CH3CN (3), can be prepared in minutes by a horizontal diffusion technique and can be harvested easily for X-ray structural studies. Compound 3, previously described as “Li2TCNQF4,” forms a one-dimensional (1D) ribbon. Compounds 1 and 2 can also be obtained as microcrystalline solids from methanolic solutions of MCl2/LiTCNQ/2ampy. Their variable-temperature magnetic studies confirmed a contribution of strongly antiferromagnetically coupled pairs of TCNQ•─ anion radicals at higher temperatures with exchange coupling J/kB = −1206 K and J/kB = −1369 K for 1 and 2, respectively, estimated using a spin dimer model. The presence of magnetically active anisotropic Ni(II) atoms with S = 1 in 1 was confirmed, and the magnetic behavior of 1, representing an infinite chain of alternating S = 1 sites and S = 1/2 dimers, was described by a spin-ring model suggesting ferromagnetic exchange coupling between Ni(II) sites and anion radicals.</dc:description><dc:date>2023</dc:date><dc:source>http://zaguan.unizar.es/record/128078</dc:source><dc:doi>10.1021/acs.cgd.3c00160</dc:doi><dc:identifier>http://zaguan.unizar.es/record/128078</dc:identifier><dc:identifier>oai:zaguan.unizar.es:128078</dc:identifier><dc:relation>info:eu-repo/grantAgreement/ES/DGA/E11-20R</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/DGA/M4</dc:relation><dc:relation>info:eu-repo/grantAgreement/ES/MICINN/PID2021-124880NB-I00</dc:relation><dc:identifier.citation>CRYSTAL GROWTH &amp; DESIGN 23, 6 (2023), 4357-4369</dc:identifier.citation><dc:rights>by</dc:rights><dc:rights>http://creativecommons.org/licenses/by/3.0/es/</dc:rights><dc:rights>info:eu-repo/semantics/openAccess</dc:rights></dc:dc>

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